Plasma Modeling refers to solving equations of motion that describe the state of a plasma. It is generally coupled with Maxwell's Equations for electromagnetic fields (or Poisson's Equation for electrostatic fields). There are several main types of plasma models: single particle, kinetic, fluid, hybrid kinetic/fluid, gyrokinetic and as system of many particles.
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The single particle model describes the plasma as individual electrons and ions moving in imposed (rather than selfconsistent) electric and magnetic fields. The motion of each particle is thus described by the Lorentz Force Law. In many cases of practical interest, this motion can be treated as the superposition of a relatively fast circular motion around a point called the guiding center and a relatively slow drift of this point.
The kinetic model is the most fundamental way to describe a plasma, resultantly producing a distribution function
where the independent variables and are position and velocity, respectively. A kinetic description is achieved by solving the Boltzmann equation or, when the correct description of longrange Coulomb interaction is necessary, by the Vlasov equation which contains selfconsistent collective electromagnetic field, or by the FokkerPlanck equation, in which approximations have been used to derive manageable collision terms. The charges and currents produced by the distribution functions selfconsistently determine the electromagnetic fields via Maxwell's equations.
To reduce the complexities in the kinetic description, the fluid model describes the plasma based on macroscopic quantities (velocity moments of the distribution such as density, mean velocity, and mean energy). The equations for macroscopic quantities, called fluid equations, are obtained by taking velocity moments of the Boltzmann equation or the Vlasov equation. The fluid equations are not closed without the determination of transport coefficients such as mobility, diffusion coefficient, averaged collision frequencies, and so on. To determine the transport coefficients, the velocity distribution function must be assumed/chosen. But this assumption can lead to a failure of capturing some physics.
Although the kinetic model describes the physics accurately, it is more complex (and in the case of numerical simulations, more computationally intensive) than the fluid model. The hybrid model is a combination of fluid and kinetic models, treating some components of the system as a fluid, and others kinetically.
In the gyrokinetic model, which is appropriate to systems with a strong background magnetic field, the kinetic equations are averaged over the fast circular motion of the gyroradius. This model has been used extensively for simulation of tokamak plasma instabilities (for example, the GYRO and Gyrokinetic ElectroMagnetic codes), and more recently in astrophysical applications.
In it model, the plasma is simulate for take in account so particles as computer can. As there is many particles in a plasma get used particle in cell (PIC) method and superparticles i.e one of this represent so particles as be necessary. Therefore is necessary get good computer or a cluster of them.
